An introductory look at how X-ray images are processed geared toward newcomers | Forum

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Sam bill
Sam bill Oct 20 '23

The technique known as single crystal X-ray diffraction is currently the one that is thought to be the most successful in terms of precisely determining the three-dimensional structure of molecules. This technique can be used on samples in biology as well as in chemistry, and the number of atoms in those samples can range anywhere from a few to many thousands. Up until this point, the scientist will have conducted practical experiments; however, after this point, everything will be purely computational, and each step can be repeated ad nauseam using a variety of programs. Given that data collection is the very last experimental step in the process, https://www.drawellanalytical.com/...-diffractometer-xrd/" _href="https://www.drawellanalytical.com/...-diffractometer-xrd/">XRD

 is of the utmost importance to put a great deal of thought, time, and effort into acquiring the very best diffraction data that is possible. This is because data collection is the very last step in the process.

Even though the majority of synchrotrons use automated systems to process the data, and even though the scientist is provided with the information required for structure solution, it is still beneficial to have an understanding of the various stages and the tasks that they perform. inIntegration is a process that can be broken down into four distinct steps, whereas scaling and merging are typically thought of as a single step. However, integration can be broken down into these steps. The step that involves scaling and merging the data is the one that generates the most helpful statistics regarding the quality of the data processing as well as the data collection. This is due to the fact that it is the step that follows the integration step, which provides a significant amount of valuable information.

Crystals are three-dimensional arrays that contain the atoms, molecules, or ions that make up the crystal's constituents. These three-dimensional arrays are also referred to as lattices. In order to form the crystal, the 'unit cell,' which is the most fundamental building block, is repeated in a translational manner across all three dimensions.


When a crystal is illuminated by radiation with a wavelength that is roughly the same as the dimensions of the unit cell (actually, within a few orders of magnitude; X-rays have a wavelength of 0 angstroms), the crystal will exhibit diffraction.


- This additional symmetry tells us that there will probably be more than one copy of the molecule in the unit cell, which is information that can be helpful when figuring out the structure of the crystal

- This information can help us figure out how the molecule is arranged within the crystal

- In addition to this, the symmetry offers us information that can be put to use in order to find a solution to the problem

- In the case of monoclinic crystals, the reflections (h,k,l) and (–h, k, –l) are interchangeable with one another; however, in the case of triclinic crystals, this is not the case



Including the components of

The term "extraction" refers to the process of obtaining the intensity information for the diffraction spots that are displayed on the images.

Exploration and enlightenment

The first thing that needs to be done in order for integration to take place is to locate a set of spots on a set of images in order for those images to be indexed. This is necessary in order for those images to be indexed., DIALS, and XDS) use spots from each of the images to ensure that they have access to additional information during later stages of the integration process. On the other hand, other methods use spots from either a single image (HKL2000) or a few images (Mosflm), and they are still able to obtain sufficient information to index successfully in the vast majority of instances. However, computer programs have to start from scratch every time in order to locate the spots; in order to do this, they use information that is typical of the majority of diffraction patterns, such as the following:

Spots that are geographically close to one another will have shapes that are comparable to one another on each image.

There are spots that are relatively powerful, spots that are relatively medium in strength, and spots that are relatively weak in strength. Because indexing only requires a sampling of spots, an intensity cut-off can be utilized to assist in the elimination of noise.


This procedure creates a three-dimensional index, as its name suggests, and it does so by giving each reflection in the dataset a unique value for each of the indices that are listed below: h, k, and l. The name of this procedure gives away some of its secrets. The Miller indices are the names that are commonly given to these numerical values. In order to successfully index, it is necessary to have accurate knowledge of the direct beam position on the detector, the distance from the crystal to the detector, and the wavelength of the radiation. Errors in any one of these factors are responsible for the majority of indexing failures at this stage in the processing.

Another piece of information that can be obtained at this point is the mosaicity, which relates to the structure of the crystal by itself. This information can be obtained right now. Diffraction spots do not occur instantaneously for a single, precise orientation of a crystal; rather, they appear and disappear through a small range of orientations. This is because of the fact that crystals have multiple faces, each of which has its own unique orientation. This is the logical conclusion that can be drawn from the prior point. crystals whose mosaicities are close to or below zero.

Enhanced alterations to the parameters

Both positional refinement and post-refinement are utilized as methods in the process of refinement. Positional refinement comes first, followed by post-refinement.

Positional refinement, which is illustrated in Figure 1a, aims to narrow the gap as much as possible between the positions of spots on the detector that have been observed and those that have been calculated to be there. This is a simple idea that can be understood without much difficulty and is not difficult to picture.